Citation: Numan Yalçın, Mutlu Dedeturk. Solutions of multiplicative ordinary differential equations via the multiplicative differential transform method[J]. AIMS Mathematics, 2021, 6(4): 3393-3409. doi: 10.3934/math.2021203
[1] | Saima Noor, Azzh Saad Alshehry, Asfandyar Khan, Imran Khan . Innovative approach for developing solitary wave solutions for the fractional modified partial differential equations. AIMS Mathematics, 2023, 8(11): 27775-27819. doi: 10.3934/math.20231422 |
[2] | Dan Chen, Da Shi, Feng Chen . Qualitative analysis and new traveling wave solutions for the stochastic Biswas-Milovic equation. AIMS Mathematics, 2025, 10(2): 4092-4119. doi: 10.3934/math.2025190 |
[3] | Raed Qahiti, Naher Mohammed A. Alsafri, Hamad Zogan, Abdullah A. Faqihi . Kink soliton solution of integrable Kairat-X equation via two integration algorithms. AIMS Mathematics, 2024, 9(11): 30153-30173. doi: 10.3934/math.20241456 |
[4] | Ziying Qi, Lianzhong Li . Lie symmetry analysis, conservation laws and diverse solutions of a new extended (2+1)-dimensional Ito equation. AIMS Mathematics, 2023, 8(12): 29797-29816. doi: 10.3934/math.20231524 |
[5] | Pengshe Zheng, Jing Luo, Shunchu Li, Xiaoxu Dong . Elastic transformation method for solving ordinary differential equations with variable coefficients. AIMS Mathematics, 2022, 7(1): 1307-1320. doi: 10.3934/math.2022077 |
[6] | Lin Fan, Shunchu Li, Dongfeng Shao, Xueqian Fu, Pan Liu, Qinmin Gui . Elastic transformation method for solving the initial value problem of variable coefficient nonlinear ordinary differential equations. AIMS Mathematics, 2022, 7(7): 11972-11991. doi: 10.3934/math.2022667 |
[7] | Yameng Duan, Wieslaw Krawcewicz, Huafeng Xiao . Periodic solutions in reversible systems in second order systems with distributed delays. AIMS Mathematics, 2024, 9(4): 8461-8475. doi: 10.3934/math.2024411 |
[8] | Keqiang Li, Shangjiu Wang . Multiple periodic solutions of nonlinear second order differential equations. AIMS Mathematics, 2023, 8(5): 11259-11269. doi: 10.3934/math.2023570 |
[9] | Awatif Muflih Alqahtani, Shahid Ahmad Wani, William Ramírez . Exploring differential equations and fundamental properties of Generalized Hermite-Frobenius-Genocchi polynomials. AIMS Mathematics, 2025, 10(2): 2668-2683. doi: 10.3934/math.2025125 |
[10] | Yang Wang, Yating Li, Yansheng Liu . Multiple solutions for a class of BVPs of fractional discontinuous differential equations with impulses. AIMS Mathematics, 2023, 8(3): 7196-7224. doi: 10.3934/math.2023362 |
Classical analysis was described by Gottfried Leibniz and Isaac Newton in the 17th century. Classical analysis consists of concepts such as limit, derivative, integral and series. Since the basis of these concepts is based on addition and subtraction, this analysis is also referred to as additive analysis.
Volterra type analysis was defined by Vito Volterra in 1887 as an alternative to classical analysis [14]. After the definition of Volterra analysis, some new studies were performed between 1967 and 1970 by Michael Grossman and Robert Katz. As a result of these studies, new analyses called geometric analysis, bigeometric analysis and anageometric analysis have been defined [12]. Some basic definitions and concepts are given about this new analysis, which is also called non-Newtonian analysis [12].
Geometric analysis, which is one of the non-Newtonian types of analysis, was first expressed by Dick Stanley as a multiplicative analysis [9]. Addition and subtraction in classical analysis corresponded to multiplication and division in geometric analysis. For this reason geometric analysis is called multiplicative calculus. In the following years, some studies on multiplicative analysis were done by Duff Campell [7]. Then, in 2008, fundamental concepts of multiplicative analysis were defined and some applications were given by Bashirov [2].
Some studies in recent years [2,3] have proven that the concept of multiplicative analysis, which has emerged as an alternative to classical analysis and offers a different perspective to problems encountered in science and engineering, has developed quite rapidly [3]. In recent years [1,4,5,6,8,10,11,15,16,17,18,19], using the basic concepts of multiplicative analysis some work was done on multiplicative ordinary differential equations.
In this study, a new transform method is introduced, namely one-dimensional multiplicative differential transform method (MDTM) and solutions of some multiplicative differential equations are investigated with the help of this method.
In this section, we will give some basic definitions and properties of the multiplicative derivative theory which can be found in [2,3,5,9].
Definition 2.1. Let f:R→R+ be a positive function. The multiplicative derivative of the function f is given by:
d∗fdx(x)=f∗(x)=limh→0(f(x+h)f(x))1/h. | (2.1) |
Assuming that f is a positive function and using properties of the classical derivative, the multiplicative derivative can be written as
f∗(x)=limh→0(f(x+h)f(x))1/h=limh→0[1+f(x+h)−f(x)f(x)](f(x)f(x+h)−f(x)f(x+h)−f(x)h1f(x))=exp(f′(x)f(x))f∗(x)=exp(ln∘f)′(x) | (2.2) |
for (ln∘f)(x)=ln[f(x)].
Definition 2.2. If the multiplicative derivative f∗ as a function also has a multiplicative derivative, then multiplicative derivative of f∗ is called second order multiplicative derivative of f and it is represented by f∗∗. Similarly, we can define nth order multiplicative derivative of f with the notation f∗(n). With n times repetition of the multiplicative differentiation operation, a positive f function has an nth order multiplicative derivative at the point x which is defined as
f∗(n)(x)=exp(ln∘f)(n)(x). | (2.3) |
Theorem 2.1. If a positive function f is differentiable with the multiplicative derivative at the point x, then it is differentiable in the classical sense and the relation between these two derivatives can be shown as
f′(x)=f(x)lnf∗(x). | (2.4) |
Theorem 2.2. Let f and g be differentiable with the multiplicative derivative. If c is an arbitrary constant, then the functions c⋅f, f⋅g, f+g, f/g, fg have multiplicative derivatives given by
1)1)(c⋅f)∗(x)=f∗(x),2)2)(f⋅g)∗(x)=f∗(x)⋅g∗(x),3)3)(f+g)∗(x)=f∗(x)f(x)f(x)+g(x)g∗(x)g(x)f(x)+g(x),4)4)(f/g)∗(x)=f∗(x)/g∗(x),5)5)(fg)∗(x)=f∗(x)g(x)f(x)g′(x). | (2.5) |
Theorem 2.3. Let g be differentiable in the multiplicative sense, h be differentiable in the classical sense. If
f(x)=(g∘h)(x), |
then, it follows that
f∗(x)=[g∗(h(x))]h′(x). | (2.6) |
Definition 2.3. A multiplicative integral is also defined in [2] for positive bounded functions and if f is Riemann integrable on [a,b], then
∗∫baf(x)dx=exp[∫ba(lnf(x))dx]=e∫ba[lnf(x)]dx. | (2.7) |
This multiplicative integral has the properties:
1)∗∫ba[f(x)k]dx=∗[∫ba(f(x))dx]k,fork∈R,2)∗∫ba[f(x)g(x)]dx=∗∫ba[f(x)]dx∗∫ba[g(x)]dx,3)∗∫ba[f(x)g(x)]dx=∗∫ba[f(x)]dx∗∫ba[g(x)]dx,4)∗∫baf(x)dx=∗∫caf(x)dx∗∫bcf(x)dx,fora≤c≤b. | (2.8) |
Multiplicative linear differential equations can be defined as in [16,17] by
(y∗(n))an(x)(y∗(n−1))an−1(x)⋯(y∗∗)a2(x)(y∗)a1(x)(y)a0(x)=f(x) | (3.1) |
Here, f(x) is a positive definite function. Multiplicative Taylor Theorem is defined as below [2,19].
f(x+h)=n∏m=0[f∗(m)(x)]hm/m![f∗(n+1)(x+θh)]hn+1/(n+1)!, for some θ∈(0,1) | (3.2) |
Definition 3.1. Let f(x) be a multiplicative analytic function with one variable. Then, for given x0 and for k∈N0, the multiplicative differential transform function F∗(k) of function f(x) is defined as
F∗(k)=[f∗(k)(x0)]1/k!. | (3.3) |
The inverse multiplicative differential transform function of F∗(k) is written as
f(x)=∞∏k=0[F∗(k)](x−x0)k,(f(x)=∞∏k=0[f∗(k)(x0)](x−x0)k/k!). | (3.4) |
Here, if we take x0=0, then
f(x)=∞∏k=0[F∗(k)]xk. | (3.5) |
The equality
f(x)=∞∏k=0[f∗(k)(0)]xk/k! | (3.6) |
is called the Taylor series with one variable. The product
∞∏k=n+1[F∗(k)]xk | (3.7) |
of remaining terms gives the truncation error and the nth degree Taylor polynomial
f(x)≈n∏k=0[F∗(k)]xk | (3.8) |
gives an approximation of f(x) for x near 0.
Lemma 3.1. If f(x)=c where c is a positive constant, then for any x0 the multiplicative differential transform of f at x0 is given by
F∗(k)={c,ifk=0,1,ifk≥1. | (3.9) |
Theorem 3.1. If λ∈R and y(x) is a multiplicative analytic function, then multiplicative differential transform of function
f(x)=[y(x)]λ | (3.10) |
is
F∗(k)=[Y∗(k)]λ. | (3.11) |
Theorem 3.2. Let y(x) and z(x) be two multiplicative analytic functions. Then the multiplicative differential transform of function f(x)=y(x)z(x) is
F∗(k)=Y∗(k)Z∗(k). | (3.12) |
Proof.
F∗(k)=[f∗(k)(x0)]1/k!=[y∗(k)(x0)z∗(k)(x0)]1/k!=Y∗(k)Z∗(k). |
Theorem 3.3. Let y(x) and z(x) be two multiplicative analytic functions. Then the multiplicative differential transform of function f(x)=y(x)/z(x) is
F∗(k)=Y∗(k)Z∗(k). | (3.13) |
Theorem 3.4. If y(x) is a multiplicative analytic function, then the multiplicative differential transform of function f(x)=y∗(x) is
F∗(k)=[Y∗(k+1)](k+1). | (3.14) |
Proof.
F∗(k)=[f∗(k)(x0)]1/k!=[(y∗)∗(k)(x0)]1/k!=[y∗(k+1)(x0)]1/k!=[y∗(k+1)(x0)](k+1)/(k+1)!=[(y∗(k+1)(x0))1/(k+1)!]k+1=[Y∗(k+1)](k+1). |
Theorem 3.5. If y(x) is a multiplicative analytic function, then the multiplicative differential transform of function f(x)=y∗∗(x) is
F∗(k)=[Y∗(k+2)](k+1)(k+2). | (3.15) |
Proof.
F∗(k)=[f∗(k)(x0)]1/k!=[(y∗∗)∗(k)(x0)]1/k!=[y∗(k+2)(x0)]1/k!=[y∗(k+2)(x0)][(k+1)(k+2)]/(k+2)!=[(y∗(k+2)(x0))1/(k+2)!](k+1)(k+2)=[Y∗(k+2)](k+1)(k+2). |
Theorem 3.6. If y(x) is a multiplicative analytic function, then the multiplicative differential transform of function f(x)=y∗(n)(x) is
F∗(k)=[Y∗(k+n)](k+n)!/k!. | (3.16) |
Theorem 3.7. Let y(x) and z(x) be two multiplicative analytic functions. Then the multiplicative differential transform of function f2(x)=z(x)lny(x)=exp{lny(x)lnz(x)} is
F∗2(k)=k∏r=0exp{lnY∗(r)lnZ∗(k−r)}. | (3.17) |
Proof.
F∗2(k)=[f∗(k)2(x0)]1/k!={[(z(x)lny(x))∗(k)]x=x0}1/k!={[(z(x)lny(x))∗k]}1/k!|x=x0={[z∗(k)(x)]lny(x)[z∗(k−1)(x)](k1)lny∗(x)⋯[z∗(k−r)(x)](kr)lny∗(r)(x)⋯[z(x)]lny∗(k)(x)}1/k!|x=x0={[z∗(k)(x0)]lny(x0)[z∗(k−1)(x)](k1)lny∗(x0)⋯[z∗(k−r)(x0)](kr)lny∗(r)(x0)⋯[z(x0)]lny∗(k)(x0)}1/k!={k∏r=0[z∗(k−r)(x0)](kr)lny∗(r)(x0)}1/k!={k∏r=0[z∗(k−r)(x0)]k!(k−r)!r!lny∗(r)(x0)}1/k!={k∏r=0[(z∗(k−r)(x0))1/(k−r)!]1r!lny∗(r)(x0)}={k∏r=0[(z∗(k−r)(x0))1/(k−r)!]ln(y∗(r)(x0))1/r!}=k∏r=0Z∗(k−r)lnY∗(r)=k∏r=0exp{lnY∗(r)lnZ∗(k−r)}. |
Theorem 3.8. Let y1(x), y2(x), and y3(x) be multiplicative analytic functions. Then the multiplicative differential transform of function
f3(x)=exp[lny1(x)lny2(x)lny3(x)] | (3.18) |
is
F∗3(k)=k∏r2=0r2∏r1=0exp[lnY∗1(r1)lnY∗2(r2−r1)lnY∗3(k−r2)]. | (3.19) |
Proof. Let's define f2(x)=exp{lny1(x)lny2(x)}. From the theorem above for the function f2(x)=exp{lny1(x)lny2(x)}, we have
F∗2(k)=k∏r1=0exp[lnY∗1(r1)lnY∗2(k−r1)]. |
Using this we can write that
f3(x)=exp{[lny1(x)lny2(x)]lny3(x)}f3(x)=exp{ln[exp{lny1(x)lny2(x)}]lny3(x)}F∗3(k)=k∏r2=0exp[lnF∗2(r2)lnY∗3(k−r2)]=k∏r2=0exp{ln(r2∏r1=0exp[lnY∗1(r1)lnY∗2(r2−r1)])lnY∗3(k−r2)}=k∏r2=0exp{(r2∑r1=0lnexp[lnY∗1(r1)lnY∗2(r2−r1)])lnY∗3(k−r2)}=k∏r2=0exp{(r2∑r1=0[lnY∗1(r1)lnY∗2(r2−r1)])lnY∗3(k−r2)}=k∏r2=0expr2∑r1=0[lnY∗1(r1)lnY∗2(r2−r1)lnY∗3(k−r2)]F∗3(k)=k∏r2=0r2∏r1=0exp[lnY∗1(r1)lnY∗2(r2−r1)lnY∗3(k−r2)]. |
Theorem 3.9. Let y1(x), y2(x), …, yn(x) be multiplicative analytic functions. Then the multiplicative differential transform of function
fn(x)=exp[lny1(x)lny2(x)…lnyn(x)] | (3.20) |
is
F∗n(k)=k∏rn−1=0rn−1∏rn−2=0...r3∏r2=0r2∏r1=0exp[lnY∗1(r1)lnY∗2(r2−r1)…lnY∗n(k−rn−1)]. | (3.21) |
Proof. We will proof this by using induction. In the theorems above we showed that it is true for n=2 and n=3.
Now, let's assume it is true for n−1 and show that it is true for n. Thus assume for
fn−1(x)=exp[lny1(x)lny2(x)…lnyn−1(x)]. | (3.22) |
we have
F∗n−1(k)=k∏rn−2=0rn−2∏rn−3=0⋯r3∏r2=0r2∏r1=0exp[lnY∗1(r1)lnY∗2(r2−r1)…lnY∗n−1(k−rn−2)]. | (3.23) |
For the function
fn(x)=exp[lny1(x)lny2(x)…lnyn−1(x)lnyn(x)]=exp[{lny1(x)lny2(x)…lnyn−1(x)}lnyn(x)]=exp{ln[exp{lny1(x)lny2(x)…lnyn−1(x)}]lnyn(x)}fn(x)=exp{ln[fn−1(x)]lnyn(x)} |
we can write
F∗n(k)=k∏rn−1=0exp[lnF∗n−1(rn−1)lnY∗n(k−rn−1)]=k∏rn−1=0exp{ln(rn−1∏rn−2=0⋯r2∏r1=0exp[lnY∗1(r1)…lnY∗n−1(rn−1−rn−2)])lnY∗n(k−rn−1)}=k∏rn−1=0exp{rn−1∑rn−2=0⋯r2∑r1=0lnexp[lnY∗1(r1)⋯lnY∗n−1(rn−1−rn−2)]lnY∗n(k−rn−1)}F∗n(k)=k∏rn−1=0rn−1∏rn−2=0⋯r2∏r1=0exp[lnY∗1(r1)…lnY∗n−1(k−rn−2)lnY∗n(k−rn−1)]. |
And this proves the theorem.
Theorem 3.10. The multiplicative differential transform of function f(x)=exp{xm} at x0=0 is
F∗(k)=δ∗(k−m)={e,fork=m1,fork≠m | (3.24) |
Proof. For k<m, we have
F∗(k)=[f∗(k)(x)]1/k!|x=0=[(exp{xm})∗(k)]1/k!|x=0=[exp{m(m−1)…(m−k+1)xm−k}]1/k!|x=0=[exp{0}]1/k!=1. |
For k=m, we have
F∗(k)=F∗(m)=[f∗(m)(x)]1/m!|x=0=[exp{m!}]1/m!|x=0=exp{m!(1/m!)}|x=0=e. |
For k>m, ∃h∈Z+such that k=m+h, and
F∗(k)=[f∗(k)(x)]1/k!|x=0=[f∗(m+h)(x)]1/(m+h)!|x=0=[{f∗(m)(x)}∗(h)]1/(m+h)!|x=0=[{exp(m!)}∗(h)]1/(m+h)!=1. |
Theorem 3.11. The multiplicative differential transform of function f(x)=exp{eλx} at x0=0 is
F∗(k)=exp{λk/k!}. | (3.25) |
Proof.
F∗(k)=[f∗(k)(x)]1/k!|x=0=[exp{λkeλx}]1/k!|x=0=[exp{eλx}]λk/k!|x=0=[exp{e0}]λk/k!=exp{λk/k!}. |
Theorem 3.12. The multiplicative differential transform of function f(x)=exp{aλx} at x0=0 is
F∗(k)=exp{(λlna)k/k!}. | (3.26) |
Proof.
F∗(k)=[f∗(k)(x)]1/k!|x=0=[exp{(λlna)kaλx}]1/k!|x=0=[exp{(λlna)k}]1/k!=exp{(λlna)k/k!}. |
Theorem 3.13. The multiplicative differential transform of function f(x)=exp{sin(ωx+α)} at x0=0 is
F∗(k)=exp{ωkk!sin(π2k+α)}. | (3.27) |
Proof.
F∗(k)=[f∗(k)(x)]1/k!|x=0=[exp{ωksin(π2k+ωx+α)}]1/k!|x=0=exp{ωkk!sin(π2k+α)}. |
Theorem 3.14. The multiplicative differential transform of function f(x)=exp{cos(ωx+α)} at x0=0 is
F∗(k)=exp{ωkk!cos(π2k+α)}. | (3.28) |
Proof.
F∗(k)=[f∗(k)(x)]1/k!|x=0=[exp{ωkcos(π2k+ωx+α)}]1/k!|x=0=exp{ωkk!cos(π2k+α)}. |
Here, we will give a theorem and its application about approximate solution of the Cauchy problem for first order linear multiplicative differential equations by the multiplicative differential transform method.
Theorem 4.1. Suppose the Cauchy problem for first order linear multiplicative differential equation
(y∗)ylnp(x)=q(x),y(0)=y0 | (4.1) |
is given. Here p(x)>0. Then the solution of this problem is obtained from the recurrence relations
Y∗(k+1)=exp{−1k+1[k∑r=0[lnY∗(r)lnP∗(k−r)]−ln{Q∗(k)}]},Y∗(0)=y0. | (4.2) |
Here the multiplicative differential transforms of y(x),p(x) and q(x) are Y∗(k),P∗(k) and Q∗(k), respectively.
Proof. Taking the multiplicative differential transform of both sides of the equation
Y∗(k+1)(k+1)k∏r=0exp[lnY∗(r)lnP∗(k−r)]=Q∗(k),ln{[Y∗(k+1)](k+1)k∏r=0exp[lnY∗(r)lnP∗(k−r)]}=ln{Q∗(k)},ln[Y∗(k+1)](k+1)+ln{k∏r=0exp[lnY∗(r)lnP∗(k−r)]}=ln{Q∗(k)},(k+1)ln[Y∗(k+1)]+lnexpk∑r=0[lnY∗(r)lnP∗(k−r)]=ln{Q∗(k)}. |
Thus we have
ln[Y∗(k+1)]=−1k+1[k∑r=0[lnY∗(r)lnP∗(k−r)]−ln{Q∗(k)}]. |
As a result, we get the recurrence relation
Y∗(k+1)=exp{−1k+1[k∑r=0[lnY∗(r)lnP∗(k−r)]−ln{Q∗(k)}]}. |
And, applying the multiplicative differential transform to y(0)=y0 we have
Y∗(0)=y0. | (4.3) |
Example 4.1. Suppose the Cauchy problem
(y∗)ylne4x=e2x,y(0)=e3/2 | (4.4) |
is given near x=0. Let's solve it by multiplicative differential transform method. First, the function p(x)=e4x has multiplicative differential transform
P∗(1)=[p∗(1)(x)]1/1!|x=0=[e(lne4x)′]1/1!|x=0=e4P∗(0)=[p(0)]1/0!|x=0=e0=1P∗(k)=[p∗(k)(0)]1/k!|x=0=11/k!=1, k=2,3,… |
The second function q(x)=e2x has multiplicative differential transform
Q∗(1)=[q∗(0)]1/1!=e2Q∗(k)=1, for k=0 or k=2,3,… |
To sum up
P∗(k)={1,for k≠1,e4,for k=1, | (4.5) |
and
Q∗(k)={1,for k≠1,e2,for k=1. | (4.6) |
Also we will use Y∗(0)=y(0)=e3/2. Thus we must solve the recurrence relations
Y∗(k+1)=exp{−1k+1[k∑r=0[lnY∗(r)lnP∗(k−r)]−ln{Q∗(k)}]},Y∗(0)=e3/2. |
For k=0 we have
Y∗(1)=exp{−10+1[0∑r=0[lnY∗(r)lnP∗(−r)]−ln{Q∗(0)}]}=exp{−([lnY∗(0)lnP∗(0)]−ln{Q∗(0)})}=exp{−[32⋅0]+0}Y∗(1)=1. | (4.7) |
For k=1 we have
Y∗(2)=exp{−12[1∑r=0[lnY∗(r)lnP∗(1−r)]−ln{Q∗(1)}]}=exp{−12[lnY∗(0)lnP∗(1)+lnY∗(1)lnP∗(0)−ln{Q∗(1)}]}=exp{−12[lne3/2lne4+ln1ln1−lne2]}=exp(−2)Y∗(2)=e−2. | (4.8) |
Thus an approximate solution of order two is
y(x)≅2∏k=0[Y∗(k)]xk=Y∗(0)[Y∗(1)]x[Y∗(2)]x2 | (4.9) |
y(x)≅e3/2⋅(e−2)x2 | (4.10) |
Theorem 5.1. Suppose the Cauchy problem for second order linear multiplicative differential equation
(y∗∗)(y∗)γ1yγ0=f(x),y(0)=y0,y∗(0)=y1 | (5.1) |
is given near x=0. Here γ0=lna0,γ1=lna1 and the multiplicative differential transforms of y(x),a0(x) and a1(x) are Y∗(k), A∗0(k) and A∗1(k), respectively. Solution of this problem is obtained by the recurrence relations below:
Y∗(k+2)=exp{lnF∗(k)−k∑r=0[(r+1)lnY∗(r+1)lnA∗1(k−r)+lnY∗(r)lnA∗0(k−r)](k+2)(k+1)}, | (5.2) |
Y∗(0)=y0,Y∗(1)=y1. | (5.3) |
Proof. Using the equalities γ1=lna1, γ0=lna0, the equation above can be written as
f(x)=(y∗∗)(y∗)lna1ylna0 |
Taking the multiplicative differential transform of both sides of the equation
F∗(k)=Y∗(k+2)(k+2)(k+1)k∏r=0exp{lnY∗(r+1)(r+1)lnA∗1(k−r)}k∏r=0exp{lnY∗(r)lnA∗0(k−r)}=Y∗(k+2)(k+2)(k+1)expk∑r=0{lnY∗(r+1)(r+1)lnA∗1(k−r)}expk∑r=0{lnY∗(r)lnA∗0(k−r)}=Y∗(k+2)(k+2)(k+1)exp(k∑r=0{lnY∗(r+1)(r+1)lnA∗1(k−r)}+k∑r=0{lnY∗(r)lnA∗0(k−r)})=Y∗(k+2)(k+2)(k+1)exp(k∑r=0{lnY∗(r+1)(r+1)lnA∗1(k−r)+lnY∗(r)lnA∗0(k−r)})=Y∗(k+2)(k+2)(k+1)k∏r=0exp{lnY∗(r+1)(r+1)lnA∗1(k−r)+lnY∗(r)lnA∗0(k−r)} |
Taking logarithm of both sides, we can write
lnF∗(k)=ln[Y∗(k+2)(k+2)(k+1)k∏r=0exp{lnY∗(r+1)(r+1)lnA∗1(k−r)+lnY∗(r)lnA∗0(k−r)}]=(k+2)(k+1)ln[Y∗(k+2)]+ln[k∏r=0exp{lnY∗(r+1)(r+1)lnA∗1(k−r)+lnY∗(r)lnA∗0(k−r)}]=(k+2)(k+1)ln[Y∗(k+2)]+lnexpk∑r=0{lnY∗(r+1)(r+1)lnA∗1(k−r)+lnY∗(r)lnA∗0(k−r)}=(k+2)(k+1)ln[Y∗(k+2)]+k∑r=0{lnY∗(r+1)(r+1)lnA∗1(k−r)+lnY∗(r)lnA∗0(k−r)} |
Thus we have
lnY∗(k+2)=lnF∗(k)−k∑r=0[(r+1)lnY∗(r+1)lnA∗1(k−r)+lnY∗(r)lnA∗0(k−r)](k+2)(k+1), |
and we get the recurrence relation
Y∗(k+2)=exp{lnF∗(k)−k∑r=0[(r+1)lnY∗(r+1)lnA∗1(k−r)+lnY∗(r)lnA∗0(k−r)](k+2)(k+1)}. |
For instance for k=0 we have
Y∗(2)=exp{12[lnF∗(0)−lnY∗(1)lnA∗1(0)−lnY∗(0)lnA∗0(0)]} |
and for k=1 we have
Y∗(3)=exp{16[lnF∗(1)−1∑r=0{(r+1)lnY∗(r+1)lnA∗1(1−r)+lnY∗(r)lnA∗0(1−r)}]}Y∗(3)=exp{16[lnF∗(1)−lnY∗(1)lnA∗1(1)−lnY∗(0)lnA∗0(1)−2lnY∗(2)lnA∗1(0)−lnY∗(1)lnA∗0(0)]} |
And, using multiplicative differential transform to y(0)=y0, y∗(0)=y1 we have
Y∗(0)=y0,Y∗(1)=y1. |
Example 5.1. Suppose the Cauchy problem
(y∗∗)(y∗)3y2=1, y(0)=e, y∗(0)=e−1 | (5.4) |
is given. Multiplicative differential transforms of a0=e2 and a1=e3 are
A∗0(k)={e2,for k=0,1,for k>0, and A∗1(k)={e3,for k=0,1,for k>0, | (5.5) |
respectively. Hence
lnA∗0(k)={2,for k=0,0,for k>0, and lnA∗1(k)={3,for k=0,0,for k>0, | (5.6) |
So, for the sum in the recurrence (5.2), namely
Y∗(k+2)=exp{lnF∗(k)−k∑r=0[(r+1)lnY∗(r+1)lnA∗1(k−r)+lnY∗(r)lnA∗0(k−r)](k+2)(k+1)} |
we have
lnA∗1(k−r)=0 and lnA∗0(k−r)=0 |
for r<k. Moreover, differential transform function of f(x)=1 is F∗(k)=1 so lnF∗(k)=0. Thus, we write
Y∗(k+2)=exp{−k∑r=0[(r+1)lnY∗(r+1)lnA∗1(k−r)+lnY∗(r)lnA∗0(k−r)](k+2)(k+1)}=exp{[(k+1)lnY∗(k+1)lnA∗1(0)+lnY∗(k)lnA∗0(0)]⋅−1(k+2)(k+1)}=exp{[3(k+1)lnY∗(k+1)+2lnY∗(k)]⋅−1(k+2)(k+1)}=exp{[ln(Y∗(k+1))3(k+1)+ln(Y∗(k))2]⋅−1(k+2)(k+1)}=exp{ln[(Y∗(k+1))3(k+1)(Y∗(k))2]⋅−1(k+2)(k+1)}=(exp{ln[(Y∗(k+1))3(k+1)(Y∗(k))2]})−1/[(k+2)(k+1)], |
and we get the recurrence relation
Y∗(k+2)={[Y∗(k+1)]3(k+1)[Y∗(k)]2}−1/[(k+2)(k+1)]. | (5.7) |
From the conditions y(0)=e, y∗(0)=e−1 we have
Y∗(0)=e,Y∗(1)=e−1 |
respectively. Hence solution will be obtained from the recurrence relations
Y∗(k+2)={[Y∗(k+1)]3(k+1)[Y∗(k)]2}−1/[(k+2)(k+1)],Y∗(0)=e,Y∗(1)=e−1. | (5.8) |
For k=0
Y∗(2)={[Y∗(1)]3[Y∗(0)]2}−1/2=(e−3e2)−1/2Y∗(2)=e1/2, | (5.9) |
For k=1
Y∗(3)={[Y∗(2)]3⋅2[Y∗(1)]2}−1/(3⋅2)=(e3e−2)−1/6Y∗(3)=e−1/6. | (5.10) |
Thus an approximate solution of order three is
y(x)≅3∏k=0[Y∗(k)]xk=Y∗(0)[Y∗(1)]x[Y∗(2)]x2[Y∗(3)]x3≅e(e−1)x(e1/2)x2(e−1/6)x3y(x)≅exp(1−x+x22−x36). | (5.11) |
In this study, we present the multiplicative differential transform method (MDTM) to find the approximate numerical solution of multiplicative ordinary differential equations. Then, we apply this new method to some multiplicative ordinary differential equations. It is observed that the MDTM is an effective method for multiplicative ordinary differential equations. Multiplicative power series solutions are obtained with the MDTM. The number of terms in the solution is increased to improve the accuracy of the obtained approximate solution. In some examples, the series solution obtained by the help of the MDTM can be written as an exact solution.
The authors would like to thank the editor and the anonymous referees for their constructive comments.
The authors declare that they have no competing interests regarding the publication of this manuscript.
[1] |
D. Aniszewska, Multiplicative Runge-Kutta method, Nonlinear Dyn., 50 (2007), 265–272. doi: 10.1007/s11071-006-9156-3
![]() |
[2] |
A. E. Bashirov, E. M. Kurpinar, A. Ozyapici, Multiplicative calculus and its applications, J. Math. Anal. Appl., 337 (2008), 36–48. doi: 10.1016/j.jmaa.2007.03.081
![]() |
[3] |
A. E. Bashirov, E. Misirli, Y. Tandogdu, A. Ozyapici, On modeling with multiplicative differential equations, Appl. Math., 26 (2011), 425–438. doi: 10.1007/s11766-011-2767-6
![]() |
[4] | A. Ozyapici, E. Misirli, Exponential approximations on multiplicative calculus, Proc. Jangjeon Math. Soc., 12 (2009), 227–236. |
[5] | A. Ozyapici, Çarpımsal Analiz ve Uygulamaları, Ege University, PhD thesis, 2009. |
[6] |
A. Ozyapici, B. Bilgehan, Finite product representation via multiplicative calculus and its applications to exponential signal processing, Numer. Algorithms, 71 (2016), 475–489. doi: 10.1007/s11075-015-0004-8
![]() |
[7] |
D. Campbell, Multiplicative calculus and student projects, PRIMUS, 9 (1999), 327–332. doi: 10.1080/10511979908965938
![]() |
[8] | D. Filip, C. Piatecki, An overview on the non-newtonian calculus and its potential applications to economics, Appl. Math. Comput., 187 (2007), 68–78. |
[9] |
D. Stanley, A multiplicative calculus, PRIMUS, 9 (1999), 310–326. doi: 10.1080/10511979908965937
![]() |
[10] |
E. Misirli, Y. Gurefe, Multiplicative Adams Bashforth Moulton methods, Numer. Algorithms, 57 (2011), 425–439. doi: 10.1007/s11075-010-9437-2
![]() |
[11] |
L. Florack, H. Assen, Multiplicative calculus in biomedical image analysis, J. Math. Imaging Vis., 42 (2012), 64–75. doi: 10.1007/s10851-011-0275-1
![]() |
[12] | M. Grossman, R. Katz, Non-Newtonian Calculus, Lee Press, Pigeon Cove, MA, 1972. |
[13] |
M. Riza, A. Ozyapici, E. Misirli, Multiplicative finite difference methods, Q. Appl. Math., 67 (2009), 745–754. doi: 10.1090/S0033-569X-09-01158-2
![]() |
[14] | V. Volterra, B. Hostinsky, Operations infinitesimales lineares, Gauthier-Villars, Paris, France, 1938. |
[15] | N. Yalcin, E. Celik, A. Gokdogan, Multiplicative Laplace transform and its applications, Optik, 127 (2016). |
[16] | N. Yalçın, E. Çelik, The solution of multiplicative non-homogeneous linear differential equations, J. Appl. Math. Comput., 2 (2018), 27–36. |
[17] | N. Yalcin, E. Celik, Solution of multiplicative homogeneous linear differential equations with constant exponentials, New Trends Math. Sci., 6 (2018), 58–67. |
[18] | N. Yalçı n, E. Çelik, Çarpımsal Cauchy-Euler ve Legendre diferansiyel denklemi, Gumushane Univ. J. Sci. Technol., 9 (2019), 382–373. |
[19] | N. Yalcin, The solutions of multiplicative Hermite differential equation and multiplicative Hermite polynomials, Rendiconti del Circolo Matematico di Palermo Series 2, (2020). |
1. | Arzu BAL, Numan YALÇIN, Mutlu DEDETÜRK, Solutions of Multiplicative İntegral Equations via The Multiplicative Power Series Method, 2022, 1302-0900, 10.2339/politeknik.1114825 | |
2. | Sertac Goktas, Muhammed Cinar, A New Type of Sturm-Liouville Equation in the Non-Newtonian Calculus, 2021, 2021, 2314-8888, 1, 10.1155/2021/5203939 | |
3. | Numan Yalcin, Multiplicative Chebyshev differential equations and multiplicative Chebyshev polynomials, 2022, 26, 0354-9836, 785, 10.2298/TSCI22S2785Y | |
4. | Sertaç GÖKTAŞ, Multiplicative Conformable Fractional Differential Equations, 2022, 1308-9080, 10.55525/tjst.1065429 | |
5. | Sinem KAYMAK, Numan YALÇIN, On Bigeometric Laplace Integral Transform, 2023, 13, 2536-4618, 2042, 10.21597/jist.1283580 | |
6. | Hatice Yalman Kosunalp, Selcuk Bas, Selahattin Kosunalp, An Efficient Solution of Multiplicative Differential Equations through Laguerre Polynomials, 2024, 16, 2073-8994, 748, 10.3390/sym16060748 | |
7. | Tuba GÜLŞEN, Some Approaches for Solving Multiplicative Second-Order Linear Differential Equations with Variable Exponentials and Multiplicative Airy’s Equation, 2023, 18, 1308-9080, 301, 10.55525/tjst.1282216 | |
8. | Tuba Gulsen, Sertac Goktas, Thabet Abdeljawad, Yusuf Gurefe, Sturm-Liouville problem in multiplicative fractional calculus, 2024, 9, 2473-6988, 22794, 10.3934/math.20241109 | |
9. | Numan YALÇIN, Ercan CELIK, A new approach for the bigeometric newton method, 2023, 11, 1694-7398, 235, 10.51354/mjen.1372839 | |
10. | Güler Başak ÖZNUR, Güher Gülçehre ÖZBEY, Yelda AYGARKÜÇÜKEVCİLİOĞLU, Rabia AKTAŞ, Miscellaneous properties of Sturm-Liouville problems in multiplicative calculus, 2023, 72, 1303-5991, 1141, 10.31801/cfsuasmas.1272953 | |
11. | Mehmet Yilmazer, Emrah Yilmaz, Sertac Goktas, Mikail Et, Multiplicative Laplace transform in q−calculus, 2023, 37, 0354-5180, 5859, 10.2298/FIL2318859Y | |
12. | Güher Gülçehre Özbey, Güler Başak Öznur, Yelda Aygar, Rabia Aktaş Karaman, Some properties of Bessel functions in multiplicative calculus, 2024, 0009-725X, 10.1007/s12215-024-01149-6 |